Relatively non-degenerate integrated decay estimates for massless Vlasov fields on Schwarzschild spacetimes
Léo Bigorgne, Renato Velozo Ruiz
TL;DR
This work studies the exterior of Schwarzschild for massless Vlasov fields, proving an integrated local energy decay (ILED) without relative degeneration by exploiting a trapping-weight φ_- and a carefully modified commutation vector field V_+^{mod}. A refined commutation framework, together with redshift and r^p-weighted energy methods, yields time-decay for the energy flux and, consequently, decay for the energy-momentum tensor and its first derivatives. The analysis hinges on a detailed phase-space/geometry approach to trapping near the photon sphere, a Lyapunov-type control near the horizon, and region-wise decompositions to manage degenerate derivatives. The results align with broader efforts to extend wave-equation decay techniques to kinetic equations on black hole backgrounds and are compatible with quasi-linear wave analyses on such spacetimes. Overall, the paper provides a robust toolkit for quantitative decay and regularity of massless Vlasov fields on Schwarzschild, with potential applications to nonlinear stability problems and to linear/nonlinear kinetic models in curved spacetimes.
Abstract
In this article, we make use of a weight function capturing the concentration phenomenon of unstable future-trapped causal geodesics. A projection $V_+$, on the tangent space of the null-shell, of the associated symplectic gradient turns out to enjoy good commutation properties with the massless Vlasov operator. This reflects that $V_+f$ decays exponentially locally near the photon sphere, for any smooth solution $f$ to the massless Vlasov equation. By identifying a well-chosen modification of $V_+$, we are able to construct a $W_{x,p}^{1,1}$ weighted norm for which any smooth solution to the massless Vlasov equation verifies an integrated local energy decay estimate without relative degeneration. Together with the $r^p$-weighted energy method of Dafermos--Rodnianski, we establish time decay for the energy norm. This norm allows for the control of the energy-momentum tensor $\mathrm{T}[f]$ as well as all its first order derivatives. The method developed in this paper is in particular compatible with approaches recently developed for the study of quasi-linear wave equations on black hole spacetimes.
